Synaptic complex formation of two retrovirus DNA attachment sites by integrase: a fluorescence energy transfer study

The integration of retroviral DNA by the viral integrase (IN) into the host genome occurs via assembled preintegration complexes (PIC). We investigated this assembly process using purified IN and viral DNA oligodeoxynucleotide (ODN) substrates (93 bp in length) that were labeled with donor (Cy3) and acceptor fluorophores (Cy5). The fluorophores were attached to the 5' 2 bp overhangs of the terminal attachment (att) sites recognized by IN. Addition of IN to the assay mixture containing the fluorophore-labeled ODN resulted in synaptic complex formation at 14 degrees C with significant fluorescence resonance energy transfer (FRET) occurring between the fluorophores in close juxtaposition (from approximately 15 to 100 A). Subsequent integration assays at 37 degrees C with the same ODN (32P-labeled) demonstrated a direct association of a significant FRET signal with concerted insertion of the two ODNs into the circular DNA target, here termed full-site integration. FRET measurements (deltaF) show that IN binds to a particular set of 3' OH recessed substrates (type I) generating synaptic complexes capable of full-site integration that, as shown previously, exhibit IN mediated protection from DNaseI digestion up to approximately 20 bp from the ODN att ends. In contrast, IN also formed complexes with nonspecific DNA ends and loss-of-function att end substrates (type II) that had significantly lower deltaF values and were not capable of full-site integration, and lacked the DNaseI protection properties. The type II category may exemplify what is commonly understood as "nonspecific" binding by IN to DNA ends. Two IN mutants that exhibited little or no integration activity gave rise to the lower deltaF signals. Our FRET analysis provided the first direct physical evidence that IN forms synaptic complexes with two DNA att sites in vitro, yielding a complex that exhibits properties comparable to that of the PIC.     

Near-infrared fluorescent oligodeoxyribonucleotide reporters for sensing NF-kappaB DNA interactions in vitro

Two types of reporters for optical sensing of NF-kappaB p50 protein-oligodeoxyribonucleotide (ODN) duplex interactions were designed and compared in vitro. The reporters were based on the effect of fluorescence resonance energy transfer (FRET) between the pair donor Cy5.5 near-infrared (NIR) fluorochrome and either 800CW emitting fluorescence dye acceptor (800CW-Cy), or a nonemitting QSY 21 dye quencher (QSY-Cy). The donor and the acceptor dyes were covalently linked to the complementary oligonucleotides, respectively: Cy dye was conjugated to 3'-thiol, whereas 800CW or QSY21 were conjugated to a hydrophilic internucleoside phosphate amino linker. The reporters were tested initially using recombinant NF-kappaB p50 protein binding assays. Both reporters were binding p50 protein, which protected oligonucleotide duplex from degradation in the presence of exonuclease.The incubation of 800CW-Cy reporter in the presence of control or IL-1beta treated human endothelial cells showed the uptake of the reporter in the cytoplasm and the nucleus. The measurement of NIR fluorescence ratio (i.e. Cy5.5/800CW) showed a partial loss of FRET and the increased Cy5.5 fluorescence in nontreated, control cells. Thus, the specific p50 binding to ODN duplex reporters affected the donor-acceptor fluorochrome pair. NF-kappaB p50 exhibited the protective effect on FRET between NIR fluorochromes linked to the complementary strands of the reporter duplex.     

A fluorescence resonance energy transfer sensor based on maltose binding protein

A fluorescence resonance energy-transfer (FRET) sensing system for maltose based on E. coli maltose binding protein (MBP) is demonstrated. The FRET donor portion of the sensing system consists of MBP modified with long wavelength-excitable cyanine dyes (Cy3 or Cy3.5). The novel acceptor portion of the sensor consists of beta-cyclodextrin (beta-CD) modified with either the cyanine dye Cy5 or the dark quencher QSY9. Binding of the modified beta-CD to dye-conjugated MBP results in assembly of the FRET complex. Added maltose displaces the beta-CD-dye adduct and disrupts the FRET complex, resulting in a direct change in fluorescence of the donor moiety. In the use of these FRET pairs, MBP dissociation values for maltose were estimated (0.14-2.90 microM). Maltose limits of detection were in the 50-100 nm range.     

Structural changes of yellow Cameleon domains observed by quantitative FRET analysis and polarized fluorescence correlation spectroscopy

Förster resonance energy transfer (FRET) is a widely used method for monitoring interactions between or within biological macromolecules conjugated with suitable donor-acceptor pairs. Donor fluorescence lifetimes in absence and presence of acceptor molecules are often measured for the observation of FRET. However, these lifetimes may originate from interacting and noninteracting molecules, which hampers quantitative interpretation of FRET data. We describe a methodology for the detection of FRET that monitors the rise time of acceptor fluorescence on donor excitation thereby detecting only those molecules undergoing FRET. The large advantage of this method, as compared to donor fluorescence quenching method used more commonly, is that the transfer rate of FRET can be determined accurately even in cases where the FRET efficiencies approach 100% yielding highly quenched donor fluorescence. Subsequently, the relative orientation between donor and acceptor chromophores is obtained from time-dependent fluorescence anisotropy measurements carried out under identical conditions of donor excitation and acceptor detection. The FRET based calcium sensor Yellow Cameleon 3.60 (YC3.60) was used because it changes its conformation on calcium binding, thereby increasing the FRET efficiency. After mapping distances and orientation angles between the FRET moieties in YC3.60, cartoon models of this FRET sensor with and without calcium could be created. Independent support for these representations came from experiments where the hydrodynamic properties of YC3.60 under ensemble and single-molecule conditions on selective excitation of the acceptor were determined. From rotational diffusion times as found by fluorescence correlation spectroscopy and consistently by fluorescence anisotropy decay analysis it could be concluded that the open structure (without calcium) is flexible as opposed to the rather rigid closed conformation. The combination of two independent methods gives consistent results and presents a rapid and specific methodology to analyze structural and dynamical changes in a protein on ligand binding.     

Fluorescence resonance energy transfer (FRET) and competing processes in donor-acceptor substituted DNA strands: a comparative study of ensemble and single-molecule data

We studied the fluorescence resonance energy transfer (FRET) efficiency of different donor-acceptor labeled model DNA systems in aqueous solution from ensemble measurements and at the single molecule level. The donor dyes: tetramethylrhodamine (TMR); rhodamine 6G (R6G); and a carbocyanine dye (Cy3) were covalently attached to the 5'-end of a 40-mer model oligonucleotide. The acceptor dyes, a carbocyanine dye (Cy5), and a rhodamine derivative (JA133) were attached at modified thymidine bases in the complementary DNA strand with donor-acceptor distances of 5, 15, 25 and 35 DNA-bases, respectively. Anisotropy measurements demonstrate that none of the dyes can be observed as a free rotor; especially in the 5-bp constructs the dyes exhibit relatively high anisotropy values. Nevertheless, the dyes change their conformation with respect to the oligonucleotide on a slower time scale in the millisecond range. This results in a dynamic inhomogeneous distribution of donor/acceptor (D/A) distances and orientations. FRET efficiencies have been calculated from donor and acceptor fluorescence intensity as well as from time-resolved fluorescence measurements of the donor fluorescence decay. Dependent on the D/A pair and distance, additional strong fluorescence quenching of the donor is observed, which simulates lower FRET efficiencies at short distances and higher efficiencies at longer distances. On the other hand, spFRET measurements revealed subpopulations that exhibit the expected FRET efficiency, even at short D/A distances. In addition, the measured acceptor fluorescence intensities and lifetimes also partly show fluorescence quenching effects independent of the excitation wavelength, i.e. either directly excited or via FRET. These effects strongly depend on the D/A distance and the dyes used, respectively. The obtained data demonstrate that besides dimerization at short D/A distances, an electron transfer process between the acceptor Cy5 and rhodamine donors has to be taken into account. To explain deviations from FRET theory even at larger D/A distances, we suggest that the pi-stack of the DNA double helix mediates electron transfer from the donor to the acceptor, even over distances as long as 35 base pairs. Our data show that FRET experiments at the single molecule level are rather suited to resolve fluorescent subpopulations in heterogeneous mixture, information about strongly quenched subpopulations gets lost.     

Imaging protein-protein interactions using fluorescence resonance energy transfer microscopy

Fluorescence resonance energy transfer (FRET) detects the proximity of fluorescently labeled molecules over distances >100 A. When performed in a fluorescence microscope, FRET can be used to map protein-protein interactions in vivo. We here describe a FRET microscopy method that can be used to determine whether proteins that are colocalized at the level of light microscopy interact with one another. This method can be implemented using digital microscopy systems such as a confocal microscope or a wide-field fluorescence microscope coupled to a charge-coupled device (CCD) camera. It is readily applied to samples prepared with standard immunofluorescence techniques using antibodies labeled with fluorescent dyes that act as a donor and acceptor pair for FRET. Energy transfer efficiencies are quantified based on the release of quenching of donor fluorescence due to FRET, measured by comparing the intensity of donor fluorescence before and after complete photobleaching of the acceptor. As described, this method uses Cy3 and Cy5 as the donor and acceptor fluorophores, but can be adapted for other FRET pairs including cyan fluorescent protein and yellow fluorescent protein.     

Development of a time-resolved fluorometric method for observing hybridization in living cells using fluorescence resonance energy transfer.

We previously showed that a specific kind of mRNA (c-fos) was detected in a living cell under a microscope by introducing two fluorescently labeled oligodeoxynucleotides, each labeled with donor or acceptor, into the cytoplasm, making them hybridize to adjacent locations on c-fos mRNA, and taking images of fluorescence resonance energy transfer (FRET) (A. Tsuji, H. Koshimoto, Y. Sato, M. Hirano. Y. Sei-Iida, S. Kondo, and K. Ishibashi, 2000, Biophys. J. 78:3260-3274). On the formed hybrid, the distance between donor and acceptor becomes close and FRET occurs. To observe small numbers of mRNA in living cells using this method, it is required that FRET fluorescence of hybrid must be distinguished from fluorescence of excess amounts of non-hybridizing probes and from cell autofluorescence. To meet these requirements, we developed a time-resolved method using acceptor fluorescence decays. When a combination of a donor having longer fluorescence lifetime and an acceptor having shorter lifetime is used, the measured fluorescence decays of acceptors under FRET becomes slower than the acceptor fluorescence decay with direct excitation. A combination of Bodipy493/503 and Cy5 was selected as donor and acceptor. When the formed hybrid had a configuration where the target RNA has no single-strand part between the two fluorophores, the acceptor fluorescence of hybrid had a sufficiently longer delay to detect fluorescence of hybrid in the presence of excess amounts of non-hybridizing probes. Spatial separation of 10-12 bases between two fluorophores on the hybrid is also required. The decay is also much slower than cell autofluorescence, and smaller numbers of hybrid were detected with less interference of cell autofluorescence in the cytoplasm of living cells under a time-resolved fluorescence microscope with a time-gated function equipped camera. The present method will be useful when observing induced expressions of mRNA in living cells.     

Multiplexed FRET to image multiple signaling events in live cells

We report what to our knowledge is a novel approach for simultaneous imaging of two different Förster resonance energy transfer (FRET) sensors in the same cell with minimal spectral cross talk. Previous methods based on spectral ratiometric imaging of the two FRET sensors have been limited by the availability of suitably bright acceptors for the second FRET pair and the spectral cross talk incurred when measuring in four spectral windows. In contrast to spectral ratiometric imaging, fluorescence lifetime imaging (FLIM) requires measurement of the donor fluorescence only and is independent of emission from the acceptor. By combining FLIM-FRET of the novel red-shifted TagRFP/mPlum FRET pair with spectral ratiometric imaging of an ECFP/Venus pair we were thus able to maximize the spectral separation between our chosen fluorophores while at the same time overcoming the low quantum yield of the far red acceptor mPlum. Using this technique, we could read out a TagRFP/mPlum intermolecular FRET sensor for reporting on small Ras GTP-ase activation in live cells after epidermal growth factor stimulation and an ECFP/Venus Cameleon FRET sensor for monitoring calcium transients within the same cells. The combination of spectral ratiometric imaging of ECFP/Venus and high-speed FLIM-FRET of TagRFP/mPlum can thus increase the spectral bandwidth available and provide robust imaging of multiple FRET sensors within the same cell. Furthermore, since FLIM does not require equal stoichiometries of donor and acceptor, this approach can be used to report on both unimolecular FRET biosensors and protein-protein interactions with the same cell.     

New donor-acceptor pair for fluorescent immunoassays by energy transfer

A novel F?rster donor-acceptor dye pair for an immunoassay based on resonance energy transfer (RET) is characterized with respect to its photophysical properties. As donor and acceptor, we chose the long-wavelength excitable cyanine dyes Cy5 and Cy5.5, respectively. Due to the perfect spectral overlap, an exceptionally high R(0) value of 68.7 A is obtained in solution. For biochemical applications, antibodies (IgG) are labeled with Cy5, while a tracer for competitive binding is synthesized by labeling bovine serum albumin (BSA) with an analyte derivative and Cy5.5. Binding the dyes to proteins at a low dye/protein ratio increases the fluorescence lifetimes and quantum yields, leading to an enhanced R(0) value of 85.2 A. At higher dye/protein ratios, the formation of nonfluorescent dimeric species causes a decrease in the fluorescence lifetime and quantum yield due to RET from monomeric dyes to dimers within one protein molecule. The F?rster distances could be calculated using the dimer absorption spectra to 83.9 and 83.6 A for Cy5 and Cy5.5, respectively. Upon binding of the Cy5-labeled IgG to the tracer, efficient quenching of Cy5 fluorescence is observed. Steady-state and time-resolved measurements reveal that approximately 50% of the quenching results in F?rster-type RET, while the residual quenching effect is caused by static quenching processes. The applicability of this dye pair is demonstrated in a homogeneous competitive immunoassay for the pesticide simazine.     

Development of a novel FRET immunosensor technique

We report on a novel technique to develop an optical immunosensor based on fluorescence resonance energy transfer (FRET). IgG antibodies were labeled with acceptor fluorophores while one of three carrier molecules (protein A, protein G, or F(ab')2 fragment) was labeled with donor fluorophores. The carrier molecule was incubated with the antibody to allow specific binding to the Fc portion. The labeled antibody-protein complex was then exposed to specific and nonspecific antigens, and experiments were designed to determine the 'in solution' response. The paper reports the results of three different donor-acceptor FRET pairs, fluorescein isothiocyanate/tetramethylrhodamine isothiocyanate, Texas Red/Cy5, and Alexa Fluor 546/Alexa Fluor 594. The effects of the fluorophore to protein conjugation ratio (F/P ratio) and acceptor to donor fluorophore ratios between the antibody and protein (A/D ratio) were examined. In the presence of specific antigens, the antibodies underwent a conformational change, resulting in an energy transfer from the donor to the acceptor fluorophore as measured by a change in fluorescence. The non-specific antigens elicited little or no changes. The Alexa Fluor FRET pair demonstrated the largest change in fluorescence, resulting in a 35% change. The F/P and A/D ratio will affect the efficiency of energy transfer, but there exists a suitable range of A/D and F/P ratios for the FRET pairs. The feasibility of the FRET immunosensor technique was established; however, it will be necessary to immobilize the complexes onto optical substrates so that consistent trends can be obtained that would allow calibration plots.     

Quantitative fluorescence resonance energy transfer measurements using fluorescence microscopy.

Fluorescence resonance energy transfer (FRET) is a technique used for quantifying the distance between two molecules conjugated to different fluorophores. By combining optical microscopy with FRET it is possible to obtain quantitative temporal and spatial information about the binding and interaction of proteins, lipids, enzymes, DNA, and RNA in vivo. In conjunction with the recent development of a variety of mutant green fluorescent proteins (mtGFPs), FRET microscopy provides the potential to measure the interaction of intracellular molecular species in intact living cells where the donor and acceptor fluorophores are actually part of the molecules themselves. However, steady-state FRET microscopy measurements can suffer from several sources of distortion, which need to be corrected. These include direct excitation of the acceptor at the donor excitation wavelengths and the dependence of FRET on the concentration of acceptor. We present a simple method for the analysis of FRET data obtained with standard filter sets in a fluorescence microscope. This method is corrected for cross talk (any detection of donor fluorescence with the acceptor emission filter and any detection of acceptor fluorescence with the donor emission filter), and for the dependence of FRET on the concentrations of the donor and acceptor. Measurements of the interaction of the proteins Bcl-2 and Beclin (a recently identified Bcl-2 interacting protein located on chromosome 17q21), are shown to document the accuracy of this approach for correction of donor and acceptor concentrations, and cross talk between the different filter units.     

Intermolecular dark resonance energy transfer (DRET): upgrading fluorogenic DNA sensing

The sensitivity of FRET-based sensing is usually limited by the spectral overlaps of the FRET donor and acceptor, which generate a poor signal-to-noise ratio. To overcome this limitation, a quenched donor presenting a large Stokes shift can be combined with a bright acceptor to perform Dark Resonance Energy Transfer (DRET). The consequent fluorogenic response from the acceptor considerably improves the signal-to-noise ratio. To date, DRET has mainly relied on a donor that is covalently bound to the acceptor. In this context, our aim was to develop the first intermolecular DRET pair for specific sensing of nucleic acid sequences. To this end, we designed DFK, a push–pull probe based on a fluorenyl π-platform that is strongly quenched in water. DFK was incorporated into a series of oligonucleotides and used as a DRET donor with Cy5-labeled complementary sequences. In line with our expectations, excitation of the dark donor in the double-labeled duplex switched on the far-red Cy5 emission and remained free of cross-excitation. The DRET mechanism was supported by time-resolved fluorescence measurements. This concept was then applied with binary probes, which confirmed the distance dependence of DRET as well as its potency in detecting sequences of interest with low background noise.     

FLIM on a wide field fluorescence microscope

Summary FLIM (Fluorescence Lifetime Imaging Microscopy) is a new tool to detect interaction between proteins. The proteins under investigation are fused with fluorescent donor and acceptor molecules. Interaction between the two proteins is accompanied by direct energy transfer from donor to acceptor (FRET), resulting in a shorter lifetime of the fluorescence emitted by the donor molecule. This change in lifetime is detected by FLIM. Fluorescence lifetime imaging can now be done on a widefield fluorescence microscope by using an attachment that is easy to install and simple to operate. The new LIFA attachment is equipped to use different excitation sources. High brightness modulated LEDs as well as lasers modulated by an Accousto Optical Modulator can be used as excitation light source. A modulated image intensifier with digital camera is used as a detector. Power supplies and signal generator are integrated in one control unit that is connected to the light source, detector and computer. All parameters for image acquisition, processing and viewing are easy accessible in the user interface of the software package that uses a modular structure. Lifetime images showing FRET in MCF7 cells with ErbB1-GFP as donor and Py72/Cy3 as acceptor that were taken at EMBL, Heidelberg are shown.     

Single-molecule three-color FRET

Fluorescence resonance energy transfer (FRET) measured at the single-molecule level can reveal conformational changes of biomolecules and intermolecular interactions in physiologically relevant conditions. Thus far single-molecule FRET has been measured only between two fluorophores. However, for many complex systems, the ability to observe changes in more than one distance is desired and FRET measured between three spectrally distinct fluorophores can provide a more complete picture. We have extended the single-molecule FRET technique to three colors, using the DNA four-way (Holliday) junction as a model system that undergoes two-state conformational fluctuations. By labeling three arms of the junction with Cy3 (donor), Cy5 (acceptor 1), and Cy5.5 (acceptor 2), distance changes between the donor and acceptor 1, and between the donor and acceptor 2, can be measured simultaneously. Thus we are able to show that the acceptor 1 arm moves away from the donor arm at the same time as the acceptor 2 arm approaches the donor arm, and vice versa, marking the first example of observing correlated movements of two different segments of a single molecule. Our data further suggest that Holliday junction does not spend measurable time with any of the helices unstacked, and that the parallel conformations are not populated to a detectable degree.     

Combination of novel green fluorescent protein mutant TSapphire and DsRed variant mOrange to set up a versatile in planta FRET-FLIM assay

Förster resonance energy transfer (FRET) measurements based on fluorescence lifetime imaging microscopy (FLIM) are increasingly being used to assess molecular conformations and associations in living systems. Reduction in the excited-state lifetime of the donor fluorophore in the presence of an appropriately positioned acceptor is taken as strong evidence of FRET. Traditionally, cyan fluorescent protein has been widely used as a donor fluorophore in FRET experiments. However, given its photolabile nature, low quantum yield, and multiexponential lifetime, cyan fluorescent protein is far from an ideal donor in FRET imaging. Here, we report the application and use of the TSapphire mutant of green fluorescent protein as an efficient donor to mOrange in FLIM-based FRET imaging in intact plant cells. Using time-correlated single photon counting-FLIM, we show that TSapphire expressed in living plant cells decays with lifetime of 2.93 ± 0.09 ns. Chimerically linked TSapphire and mOrange (with 16-amino acid linker in between) exhibit substantial energy transfer based on the reduction in the lifetime of TSapphire in the presence of the acceptor mOrange. Experiments performed with various genetically and/or biochemically known interacting plant proteins demonstrate the versatility of the FRET-FLIM system presented here in different subcellular compartments tested (cytosol, nucleus, and at plasma membrane). The better spectral overlap with red monomers, higher photostability, and monoexponential lifetime of TSapphire makes it an ideal FRET-FLIM donor to study protein-protein interactions in diverse eukaryotic systems overcoming, in particular, many technical challenges encountered (like autofluorescence of cell walls and fluorescence of pigments associated with photosynthetic apparatus) while studying plant protein dynamics and interactions.Single- and dual-color fluorescence imaging with intrinsically fluorescent proteins is increasingly being used to study the expression, targeting, colocalization, turnover, and associations of diverse proteins involved in different plant signal transduction pathways (for review, see Fricker et al., 2006). Concurrent with the use of fluorescence-based cell biology, Förster resonance energy transfer (FRET) has emerged as a convenient tool to study the dynamics of protein associations in vivo. The technique exploits the biophysical phenomenon of nonradiative energy transfer from a donor fluorophore to an appropriately positioned acceptor at a nanometer scale (1–10 nm; Jares-Erijman and Jovin, 2003). In living cells, FRET occurs when two proteins (or different domains within a single protein) fused to suitable donor and acceptor fluorophores physically interact, thus bringing the donor and the acceptor within the favorable proximity for energy transfer (Immink et al., 2002; Bhat et al., 2006). This results in a decrease in the donor''s fluorescence intensity (or quantum yield [QY]) and excited-state lifetime (Gadella et al., 1999). Furthermore, if the acceptor molecule is a fluorophore, then FRET additionally results in an increase in the acceptor''s emission intensity (sensitized emission; Shah et al., 2001; Bhat et al., 2006).However, the exploitation and use of fluorescent marker proteins to study protein trafficking and associations in plants can be problematic because plant cells contain a number of autofluorescent compounds (e.g. lignin, chlorophyll, phenols, etc.) whose emission spectra interfere with that of the most commonly used green or red fluorescent protein fluorophores and/or their spectral variants. For example, lignin fluorescence in roots, vascular tissues, and cell walls of aerial plant parts interferes with imaging at wavelengths between 490 and 620 nm, whereas the chlorophyll autofluorescence in green aerial plant parts is prevalent between 630 and 770 nm (Chapman et al., 2005). Consequently, conventional imaging of GFP and its closest spectral variants (like cyan fluorescent protein [CFP] and yellow fluorescent protein [YFP]) is most likely to be problematic in roots, whereas red-shifted intrinsic fluorescent proteins (including monomeric red fluorescent protein and recently identified spectral variants like mStrawberry and mCherry) may be hard to discriminate in chloroplast-containing aerial tissues (Chapman et al., 2005). The problems get further compounded in FRET assays because the autofluorescence arising from phenols, lignin, and chlorophyll can limit the choice of fluorophores suitable for in planta FRET assays.CFP and YFP have been widely used as a donor-acceptor pair in in planta FRET measurements (Bhat et al., 2006; Dixit et al., 2006). However, in photophysical terms, this pair is less than ideal for FRET imaging. Both have broad excitation and emission spectra with a small Stokes shift (Chapman et al., 2005). Second, QY of CFP (QY = 0.4) is relatively lower than that of YFP (QY = 0.61), and thus a significantly higher (and rather cell damaging) amount of excitation energy is needed to induce FRET (Dixit et al., 2006). Additionally, CFP displays multiexponential lifetimes with a shorter (1.3 ns) and a longer (2.6 ns) component (Becker et al., 2006). Although the deviation from the single-component decay is reasonably small (Tramier et al., 2002; Becker et al., 2006), the shorter CFP lifetime component can erroneously be interpreted as being the result of lifetime reduction due to energy transfer. At the same time, weak or transient protein associations may get masked and thus remain undetected. Whereas the parental wild-type GFP is extremely photostable and shows a monoexponential decay pattern (excited-state lifetime 3.16 ± 0.03 ns; Striker et al., 1999; Volkmer et al., 2000; Shaner et al., 2005), its close spectral overlap with YFP makes it unsuitable as a donor in GFP-YFP FRET experiments. Likewise, wild-type or enhanced GFP (or YFP) as a donor to red-shifted monomers as acceptors is suboptimal because the 488-nm (or 514-nm) laser line commonly used to excite GFP (or YFP) cross excites most of the red monomers (e.g. mOrange, mStrawberry) because of their broad excitation spectra (Zapata-Hommer and Griesbeck, 2003; Shaner et al., 2004).Recently, TSapphire (Q69M/C70P/V163A/S175G; excitation/emission 399/511 nm), a variant of the Sapphire (T203I) mutant of wild-type GFP with improved folding properties and better pH sensitivity, was described (Zapata-Hommer and Griesbeck, 2003). The T203I mutation in TSapphire (and original Sapphire as well) abolishes the 475-nm excitation peak found in the wild-type GFP (Tsien, 1998). TSapphire is efficiently excited below 410 nm, which makes it ideal for studying plant protein dynamics and interactions because, at this wavelength, there is negligible excitation of the autofluorescing chlorophyll pigments. Furthermore, TSapphire also represents a good donor to red monomer acceptors that are negligibly excited at this wavelength (Shaner et al., 2004). Using a purified Zn²⁺ sensor with TSapphire and mOrange as a donor-acceptor pair, Shaner and colleagues demonstrated the ratiometric intramolecular FRET between the two fluorophores in vitro (Shaner et al., 2004). The sensor yielded a 6-fold ratiometric increase (562/514-nm mOrange/TSapphire emission ratio) upon Zn²⁺ binding.However, currently there are no reports demonstrating the application and use of TSapphire and monomeric red-shifted fluorophores as donor-acceptor FRET pairs to probe intermolecular protein-protein interactions in vivo. In this article, we demonstrate in vivo FRET-fluorescence lifetime imaging microscopy (FLIM) between the donor TSapphire and the acceptor mOrange. We show that TSapphire expressed in living plant cells decays with a monoexponential lifetime of 2.93 ± 0.09 ns, which is in agreement with the published lifetime for its parent wild-type GFP (3.2 ns; Striker et al., 1999; Volkmer et al., 2000). Furthermore, we demonstrate intramolecular FRET-FLIM between chimerically linked TSapphire and mOrange (with a 16-amino acid linker in between). When fused to genetically known interacting proteins and expressed in intact living cells, the donor and the acceptor fluorophores show energy transfer in different subcellular compartments indicative of intermolecular protein-protein interactions. These results validate the versatility of the proposed in vivo FRET-FLIM assay based on the donor TSapphire and the acceptor mOrange, which turns out to work with both soluble and membrane proteins.     

Detection of frequency resonance energy transfer pair on double-labeled microsphere and Bacillus anthracis spores by flow cytometry

Development of an ultrasensitive biosensor for biological hazards in the environment is a major need for pollutant control and for the detection of biological warfare. Fluorescence methods combined with immunodiagnostic methods are the most common. To minimize background noise, arising from the unspecific adsorption effect, we have adapted the FRET (frequency resonance energy transfer) effect to the immunofluorescence method. FRET will increase the selectivity of the diagnosis process by introducing a requirement for two different reporter molecules that have to label the antigen surface at a distance that will enable FRET. Utilizing the multiparameter capability of flow cytometry analysis to analyze the double-labeling/FRET immunostaining will lead to a highly selective and sensitive diagnostic method. This work examined the FRET interaction of fluorescence-labeled avidin molecules on biotin-coated microspheres as a model system. As target system, we have used labeled polyclonal antibodies on Bacillus anthracis spores. The antibodies used were purified immunoglobulin G (IgG) molecules raised in rabbits against B. anthracis exosoporium components. The antibodies were fluorescence labeled by a donor-acceptor chromophore pair, alexa488 as a donor and alexa594 as an acceptor. On labeling the spores with alexa488-IgG as a donor and alexa594-IgG as an acceptor, excitation at 488 nm results in quenching of the alexa-488 fluorescence (E(q) = 35%) and appearance of the alexa594 fluorescence (E(s) = 22%), as detected by flow cytometry analysis. The FRET effect leads to a further isolated gate (FL1/FL3) for the target spores compared to competitive spores such as B. thuringiensis subsp. israelensis and B. subtilis. This new approach, combining FRET labeling and flow cytometry analysis, improved the selectivity of the B. anthracis spores by a factor of 10 with respect to B. thuringiensis subsp. israelensis and a factor of 100 with respect to B. subtilis as control spores.     

Correcting confocal acquisition to optimize imaging of fluorescence resonance energy transfer by sensitized emission

Imaging of fluorescence resonance energy transfer (FRET) between suitable fluorophores is increasingly being used to study cellular processes with high spatiotemporal resolution. The genetically encoded Cyan (CFP) and Yellow (YFP) variants of Green Fluorescent Protein have become the most popular donor and acceptor pair in cell biology. FRET between these fluorophores can be imaged by detecting sensitized emission. This technique, for which CFP is excited and transfer is detected as emission of YFP, is sensitive, fast, and straightforward, provided that proper corrections are made. In this study, the detection of sensitized emission between CFP and YFP by confocal microscopy is optimized. It is shown that this FRET pair is best excited at 430 nm. We identify major sources of error and variability in confocal FRET acquisition including chromatic aberrations and instability of the excitation sources. We demonstrate that a novel correction algorithm that employs online corrective measurements yields reliable estimates of FRET efficiency, and it is also shown how the effect of other error sources can be minimized.     

Modelling Förster resonance energy transfer (FRET) using anisotropy resolved multi-dimensional emission spectroscopy (ARMES)

BackgroundFörster Resonance Energy Transfer (FRET) is widely used to study the structure and dynamics of biomolecular systems and also causes the non-linear fluorescence response observed in multi-fluorophore proteins. Accurate FRET analysis, in terms of measuring changes in donor and acceptor spectra and energy transfer efficiency is therefore critical.MethodsWe demonstrate a novel quantitative FRET analysis using anisotropy resolved multidimensional emission spectroscopy (ARMES) in a Human Serum Albumin (HSA) and 1,8-anilinonaphathalene sulfonate (ANS) model. ARMES combines 4D measurement of polarized excitation emission matrices (pEEM) with multivariate data analysis to spectrally resolve contributing fluorophores. Multivariate analysis (Parallel Factor, PARAFAC and restricted Tucker3) was used to resolve fluorophore contributions and for modelling the quenching of HSA emission and the HSA-ANS interactions.ResultspEEM spectra were modelled using Tucker3 which accommodates non-linearities introduced by FRET and a priori chemical knowledge was used to optimise the solution, thus resolving three components: HSA emission, ANS emission from indirect FRET excitation, and ANS emission from direct excitation. Perpendicular emission measurements were more sensitive to indirectly excited acceptor emission. PARAFAC modelling of HSA, donor emission, separated ANS FRET interacting (Tryptophan) and non-interacting (Tyrosine) components. This enabled a new way of calculating quenching constants using the multi-dimensional emission of individual donor fluorophores.ConclusionsFRET efficiency could be calculated using the multi-dimensional, resolved emission of the interacting donor fluorophores only which yielded higher ET efficiencies compared to conventional methods.General significanceShows the potential of multidimensional fluorescence measurements and data analysis for more accurate FRET modelling in proteins.     

Confocal microscopic dual-laser dual-polarization FRET (2polFRET) at the acceptor side for correlating rotations at different distances on the cell surface

Relationship of donor and acceptor fluorescence anisotropies as well as efficiency of fluorescence resonance energy transfer (FRET) has been investigated in a confocal microscope in the context of FRET systems comprised of donor and acceptor-labeled MHCI and MHCII receptors on the surface of Kit-225 K6 human T-cells. The measurements have been carried out in a 2-laser, 5-signal platform where the total donor fluorescence intensity and 2 acceptor fluorescence intensities with their anisotropies – one at the donor's excitation wavelength, the other at the acceptor's excitation wavelength – have been detected. This configuration enabled the determination of FRET efficiency and correlating it with the two acceptor fluorescence anisotropies as a kind of calibration. Estimations for the FRET-enhanced donor fluorescence anisotropy, the directly excited acceptor fluorescence anisotropy, and the fluorescence anisotropy of sensitized emission have been obtained. Procedures for determining FRET by measuring only the total donor intensity and the acceptor intensity and its anisotropy, or two acceptor intensities and their anisotropies have been elaborated, the errors of which have been estimated based on the fluorescence anisotropy values obtained in the calibration with the method of flow cytometric energy transfer (FCET).The combined detection of the donor and acceptor fluorescence anisotropies enabled also the determination of the lower and upper limits of the orientation factor for FRET (κ²). An increase in range for κ² with increasing FRET efficiency has been observed, with average κ² values different from the dynamic random average of 2/3. These observations call for the need of κ² determination in proximity measurements, where the donor and acceptor orientations are not predictable.An increasing range of κ² with increasing intermolecular proximity of the MHCI and MHCII receptors has been observed. This indicates that molecular flexibility in the clusters of the MHCI and MHCII receptors reduces with increasing cluster density, i.e. a “fluidity gradient” exists in the clusters. More specifically, the local density dependent flexibility can also be taken as a direct proof for that the association of these receptors is non-random, but mediated by some type of physical interaction, a finding as a benefit of FRET detection by polarization spectroscopy.Two new quantities – the quenched donor fluorescence anisotropy and a fluorescence anisotropy analogue, the “dissymmetry index” of the polarized FRET efficiency components – have also been introduced for the characterization of the orientational dynamics of the excited state during FRET.